WFIRST Dark Energy

Dark Energy

  • Introduction
  • Dark Energy and the Universe
  • Measuring Dark Energy
  • WFIRST's Primary Dark Energy Science Objective: Determine the expansion history of the Universe and the growth history of its largest structures in order to test possible explanations of its apparent accelerating expansion including Dark Energy and modifications to Einstein's gravity (Green et al 2011).

    Click for a larger image
    Estimated distribution of dark matter and dark energy in the universe.
    Image Credit: NASA

    The history, geometry, and future of the Universe are determined by its composition. Our current understanding is that the Universe is 73% Dark Energy, 23% Dark Matter, and almost 4% Hydrogen and Helium. Everything else (including us!) accounts for less than 1%.

    Revolutionary observations in the past two decades have shown that the expansion of the Universe is accelerating. Dark Energy is the proposed explanation for this acceleration. The nature of dark energy, however, remains a mystery. Alternately, the acceleration may be evidence of a breakdown in Einstein's theory of gravity on cosmic scales. In either case, the cause and history of cosmic acceleration is one of the most fundamental questions in physics today.

     

    Dark Energy and the Universe

    Gravity has the effect of slowing the expansion of the Universe, while dark energy has the opposite effect. It exerts negative pressure, accelerating the expansion. These competing effects also determine how structures of dark matter and of galaxies grow.

    Image Credit: NASA/CXC/M.Weiss

    The dark energy "equation of state" is expressed as:

    w=p/ρ

    Observations show that w is close to -1 at the present time.

    If w is constant and equal to -1 the dark energy is described as a cosmological constant γ, first postulated by Einstein. WFIRST will help us to learn whether dark energy was constant over time or is more complex and has evolved.

    The future value of w also tells us the future fate of the Universe. For -1 < w < -1/3, the Universe will undergo eternal expansion. Eventually other galaxies will disappear beyond the horizon, no longer visible as the speed of light is insufficient to reach us as the Universe expands. For w < -1, the dark energy density will become infinite. Even gravitationally bound structures would be torn apart.

    Measuring Dark Energy

    In order to understand the nature of dark energy, WFIRST will measure the expansion history of the Universe and the growth of large-scale structure (the clustering of galaxies and their associated halos of dark matter in the Universe). It will use three complementary techniques:

  • Supernova Ia (SNe): "standard candles" that measure the expansion history
  • Weak Gravitational Lensing (WL): determine the expansion history and the growth of structure simultaneously, by measuring the distribution of dark matter structures through their effect on the light from distant galaxies.
  • Baryon Acoustic Oscillations (BAO): use the clustering scale of galaxies as a "standard ruler" to measure the expansion history. The same data used to examine BAO will tell us further information about the growth of structure via measurements of the local velocities of galaxies, a phenomenon referred to as Redshift Space Distortions (RSD).
  • The 2010 National Research Council New Worlds, New Horizon Decadal Survey of Astronomy and Astrophysics report stated: "Why should WFIRST employ all three methods? Supernovae (in particular, type SNe Ia) give the best measurements of cosmic acceleration parameters at low redshift due to their greater precision per sample or per object. BAO excels over large volumes at higher redshift. Together SNe Ia and BAO provide the most precise measurements of the expansion history for 0 < z < 2 and place significant constraints on the equation of state. Weak-lensing provides a complementary measurement through the growth of structure. Comparing weak-lensing results with those from supernovae and BAO could indicate that cosmic acceleration is actually a manifestation of a scale-dependent failure of general relativity. Combining all three tests provides the greatest leverage on cosmic acceleration questions. WFIRST can do all three."

    Standard Candles and Standard Rulers

    In cosmology, we derive distances from "standard candles" - objects of known intrinsic brightness. We observe how bright the object appears to be to us, and comparing that to the intrinsic brightness, we derive the distance. We can also understand the expansion history using "standard rulers" - known intrinsic separation between objects.

     

    Dark Matter

    Click for a larger image
    Image Credit: NASA,ESA, Caltech; R. Massey

    Dark matter comprises the bulk of the mass of the Universe, yet is notoriously difficult to study. This is due to the fact that dark matter neither absorbs or emits light (thus earning the moniker "dark"). Dark matter is therefore detected by its gravitational influence on luminous sources such as galaxies. In the past, evidence for dark matter has come from measuring the rotational curves of galaxies and from measuring the relative velocities of galaxies in clusters. In both cases, it is apparent that there is much more mass than what we can see in the form of stars, dust, and other forms of "normal" matter. More recently, even more conclusive evidence for dark matter has come from gravitational lensing, the distortion of the apparent shapes of background objects by foreground dark matter; this gravitational bending of light is a direct consequence of Einstein's General Theory of Relativity.

     

    Supernovae 1a

    SNe Ia are luminous "signposts," that can be observed even in distant galaxies. For this reason, they had for decades been identified as possible "standard candles" to probe the high redshift Universe for cosmology. SNe Ia are, with some confidence, thought to be the thermonuclear deflagration, or delayed detonation, of a carbon-oxygen white dwarf star, following the landmark theoretical "W7 model" by Ken'ichi Nomoto and collaborators in 1984. What promotes the white dwarf to explode is currently still unknown, but is suspected to be either mass accretion from a dwarf or giant star companion in a binary system, or the merger with its white dwarf binary companion. SNe Ia have long been found to have quite similar peak luminosities, but the dispersion around the mean of these luminosities is uncomfortably large to be considered a precise standard candle. It was realized, in 1977 by Yuri Pskovskii and, later, in 1993 by Mark Phillips and confirmed in 1996 by Mario Hamuy and collaborators, that the peak luminosities of these SNe was correlated with their rates of decline from maximum light. Several investigators since then, including Adam Riess, Saul Perlmutter, Robert Knop, and Saurabh Jha, among others, have developed relations between luminosity and decline rate, making SNe Ia "standardizable candles." Employing these relations, Brian Schmidt and Perlmutter headed up two independent teams to pursue measurement of cosmological parameters, using combined nearby and distant SNe Ia samples. The results were publications in 1998 by Schmidt and Riess, and in 1999 by Perlmutter, which showed, astonishingly, that the most distant SNe Ia were apparently fainter than they were expected to be in a matter-dominated, decelerating Universe. This could only be true if the Universe were actually accelerating locally! SNe Ia were therefore first to reveal the Accelerating Universe and the requisite for Dark Energy to explain this acceleration. Still to be fully determined are, e.g., the roles of dust extinction, evolution of SN Ia color and luminosity, and progenitor properties, as a function of redshift. Several research groups, including the CFHT SN Legacy Survey, ESSENCE, and PANS, have continued, through the increase in numbers of and distances to SNe Ia, to refine measurements of the various parameters, particularly, w, in concordance with other Dark Energy probes.

    The Type Ia SN 1994ae, discovered by S. Van Dyk and the Leuschner Observatory Supernova Search (IAU Circular 6105) on Nov. 14, 1994, in the nearby spiral galaxy NGC 3370. This image is from the 1.2-meter telescope at the Fred Lawrence Whipple Observatory and was obtained in good conditions a few weeks after maximum light. The supernova peaked at ~13th magnitude in the visual. Extensive monitoring of the light curve in 5 colors was obtained beginning 2 weeks before maximum and provides one of the most complete photometric records of a supernova light curve
    Image Credit: NASA and A. Riess (STScI)

    Click for a larger image
    Joint confidence intervals derived from SN samples for a two-parameter model of the equation-of-state parameter of dark energy, w(z) = w_a + w_a*(z/(1+z)), where z is redshift. For each panel, constraints from a SN sample are combined with the indicated prior to yield the indicated confidence intervals. The position of a cosmological constant is shown as a filled symbol.
    Image Credit: Riess et al. (2007, ApJ, 659, 98; Copyright 2007, the American Astronomical Society

     

    Weak Gravitational Lensing

    Image Credit: Jason Rhodes (JPL)

    The light from distant galaxies travels through dark matter structures along its journey to our telescopes. As a consequence of General Relativity, the path of the light is distorted by the gravitational influence of the dark matter, resulting in distortions to the observed shapes of these galaxies. By looking for small, coherent distortions of galaxies shapes, we can piece together the dark matter distribution along the line of sight to these distance galaxies. The evolution of these dark matter structures over cosmic time is driven by an interplay between the attractive force of gravity and the repulsive dark matter. Thus, by observing the growth of these dark matter structures at a range of distances (corresponding to a range in time) we can understand dark energy and gravity.

    Baryonic Acoustic Oscillations

    Large-scale redshift-space correlation function of the SDSS LRG sample, plotting the correlation function times s^2. The models are Omega_m h^2 = 0.12 (green line), 0.13 (red line), and 0.14 (blue line), all with Omega_b h^2 = 0.024 and n = 0.98 and with a mild nonlinear prescription folded in. The magenta line shows a pure CDM model (Omega_m h^2 = 0.105), which lacks the acoustic peak.
    Image Credit: Eisenstein et al., 2005 ApJ, 633, Copyright 2005, the American Astronomical Society.

    The early Universe was much hotter and denser than the Universe we see today. There were no stable atoms, only a hot plasma of electrons, protons, photons, and dark matter. Sounds waves could travel through this plasma, like the ripples on a pond. The speed of sound, then, determined a characteristic scale.

    By 370,000 years after the Big Bang, the Universe had expanded and cooled sufficiently that photons no longer had enough energy to break apart Hydrogen atoms. This change, called "recombination", fixed the distance scale imposed by the sound speed in the plasma before. Small fluctuations in the matter density (1 part in 10,000) grew into the large structures in the Universe.

    At that time, the Universe became transparent, and the photons could now travel unimpeded but shifted to longer wavelengths by the expansion of the universe. These photons today are the Cosmic Microwave Background. Measurement by WMAP and soon Planck provide a precise determination of the characteristic scale in the Early Universe.

    The distribution of galaxies allows us to measure this characteristic scale at later epochs, and serves as a "standard ruler". The technique of using the small fluctuations in the early Universe, as determined by the sound speed, as a ruler is known as Baryonic Acoustic Oscillations.

    The Sloan Digital Sky Survey provided spectacular confirmation of this prediction. By measuring the galaxy correlation function for ~50,000 galaxies, SDSS determined the most likely distance between galaxies, which results from the BAO, is the equivalent of 480 million light years today. This result confirmed the basic picture of structure formation through gravity, and the necessity of dark energy (without it the scale would have been smaller).

    Other Science Topics:

  • Exoplanet Microlensing
  • Large Area Near Infrared Surveys